20,354 research outputs found

    A classification of 3+1D bosonic topological orders (I): the case when point-like excitations are all bosons

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    Topological orders are new phases of matter beyond Landau symmetry breaking. They correspond to patterns of long-range entanglement. In recent years, it was shown that in 1+1D bosonic systems there is no nontrivial topological order, while in 2+1D bosonic systems the topological orders are classified by a pair: a modular tensor category and a chiral central charge. In this paper, we propose a partial classification of topological orders for 3+1D bosonic systems: If all the point-like excitations are bosons, then such topological orders are classified by unitary pointed fusion 2-categories, which are one-to-one labeled by a finite group GG and its group 4-cocycle Ο‰4∈H4[G;U(1)]\omega_4 \in \mathcal H^4[G;U(1)] up to group automorphisms. Furthermore, all such 3+1D topological orders can be realized by Dijkgraaf-Witten gauge theories.Comment: An important new result "Untwisted sector of dimension reduction is the Drinfeld center of E" is added in Sec. IIIC; other minor refinements and improvements; 23 pages, 10 figure

    A theory of 2+1D fermionic topological orders and fermionic/bosonic topological orders with symmetries

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    We propose that, up to invertible topological orders, 2+1D fermionic topological orders without symmetry and 2+1D fermionic/bosonic topological orders with symmetry GG are classified by non-degenerate unitary braided fusion categories (UBFC) over a symmetric fusion category (SFC); the SFC describes a fermionic product state without symmetry or a fermionic/bosonic product state with symmetry GG, and the UBFC has a modular extension. We developed a simplified theory of non-degenerate UBFC over a SFC based on the fusion coefficients NkijN^{ij}_k and spins sis_i. This allows us to obtain a list that contains all 2+1D fermionic topological orders (without symmetry). We find explicit realizations for all the fermionic topological orders in the table. For example, we find that, up to invertible p+ipp+\hspace{1pt}\mathrm{i}\hspace{1pt} p fermionic topological orders, there are only four fermionic topological orders with one non-trivial topological excitation: (1) the K=(βˆ’1002)K={\scriptsize \begin{pmatrix} -1&0\\0&2\end{pmatrix}} fractional quantum Hall state, (2) a Fibonacci bosonic topological order 214/5B2^B_{14/5} stacking with a fermionic product state, (3) the time-reversal conjugate of the previous one, (4) a primitive fermionic topological order that has a chiral central charge c=14c=\frac14, whose only topological excitation has a non-abelian statistics with a spin s=14s=\frac14 and a quantum dimension d=1+2d=1+\sqrt{2}. We also proposed a categorical way to classify 2+1D invertible fermionic topological orders using modular extensions.Comment: 23 pages, 8 table
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